3 research outputs found
ΠΠ‘ΠΠΠΠΠΠΠ‘Π’Π ΠΠΠΠΠ’Π ΠΠΠΠ₯ΠΠΠΠΠΠ£Π‘Π’ΠΠ§ΠΠ‘ΠΠΠΠ ΠΠ ΠΠΠΠ ΠΠΠΠΠΠΠΠ― ΠΠΠΠ ΠΠΠ Π¦ΠΠΠΠΠΠ ΠΠ§ΠΠ‘ΠΠΠΠ ΠΠ¬ΠΠΠΠΠΠ ΠΠΠΠ§ΠΠ‘ΠΠΠΠ ΠΠΠΠ£Π§ΠΠ’ΠΠΠ―ΠΠ Π‘ ΠΠΠ£Π’Π ΠΠΠΠΠΠ ΠΠΠ ΠΠΠΠΠ Π Π‘ΠΠ‘Π’ΠΠΠ ΠΠΠΠ‘ΠΠΠ₯ Π‘ΠΠ‘Π’ΠΠ
The problem of sound emission is considered by a system formed from cylindrical piezoceramic radiators with internal acoustically soft screens. Longitudinal axis of emitters lie in one plane. This system is characterized by the interaction of electric, mechanical and acoustic fields in the process of conversion electrical energy to acoustical energy and acoustic fields in the process of forming them in the environments. The purpose of the work is to determine the peculiarities of the electromechanical acoustic transformation of energy by cylindrical piezoceramic radiators with internal screens in the composition of flat systems, taking into account all types of interaction.The research was carried out by the method of bound fields in multiply connected domains with the use of addition theorems for the cylindrical wave functions. The physical fields arising from the emission of sound by such a system are determined by the joint solution of the system of differential equations: the wave equation; equations of motion of thin piezoceramic shells with circular polarization in displacements; the equations of forced electrostatics for piezoceramics at given boundary conditions, the conditions of conjugation of fields at the boundaries of the division of domains and electric conditions.The solution of the problem is reduced to the solution of an infinite system of linear algebraic equations with respect to unknown coefficients of field expansions.An analysis of the results of numerical calculations, performed on the basis of the obtained analytical relations, called to establish a number of features in the electromechanical acoustic transformation of energy by emitters in the composition of flat systems. They include: the role of acoustic interaction in the process of energy conversion; determination of the mechanism of quantitative assessment of the influence of interaction on these processes; the dependence of the degree of violation of the radial symmetry of the acoustic loading of the emitters on the amount of acoustic interaction; the appearance of multimodality of the mechanical field of emitters in the structure of the plane system and the dependence of the redistribution of energy between all modes on the degree of disturbance of the radial symmetry of the acoustic loading of the emitters.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Π° Π·Π°Π΄Π°ΡΠ° ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π·Π²ΡΠΊΠ° ΠΏΠ»ΠΎΡΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠΎΠΉ, ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΈΠ· ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ Ρ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠΌΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈ ΠΌΡΠ³ΠΊΠΈΠΌΠΈ ΡΠΊΡΠ°Π½Π°ΠΌΠΈ. ΠΡΠΎΠ΄ΠΎΠ»ΡΠ½ΡΠ΅ ΠΎΡΠΈ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ ΠΏΠ°ΡΠ°Π»Π»Π΅Π»ΡΠ½Ρ ΠΈ Π»Π΅ΠΆΠ°Ρ Π² ΠΎΠ΄Π½ΠΎΠΉ ΠΏΠ»ΠΎΡΠΊΠΎΡΡΠΈ. Π£ΠΊΠ°Π·Π°Π½Π½Π°Ρ ΡΠΈΡΡΠ΅ΠΌΠ° Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅ΡΡΡ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
, ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»ΡΠΌΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π² Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΡΡ ΠΈ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΎΠΊΡΡΠΆΠ°ΡΡΠΈΡ
ΡΡΠ΅Π΄Π°Ρ
. Π¦Π΅Π»ΡΡ ΡΠ°Π±ΠΎΡΡ ΡΠ²Π»ΡΠ»ΠΎΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠ΅ΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ΅Ρ
Π°Π½ΠΎΠ°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»ΡΠΌΠΈ Ρ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠΌΠΈ ΡΠΊΡΠ°Π½Π°ΠΌΠΈ Π² ΡΠΎΡΡΠ°Π²Π΅ ΠΏΠ»ΠΎΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ Ρ ΡΡΠ΅ΡΠΎΠΌ Π²ΡΠ΅Ρ
Π²ΠΈΠ΄ΠΎΠ² Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ²ΡΠ·Π°Π½Π½ΡΡ
ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΌΠ½ΠΎΠ³ΠΎΡΠ²ΡΠ·Π½ΡΡ
ΠΎΠ±Π»Π°ΡΡΡΡ
Ρ ΠΏΡΠΈΠ²Π»Π΅ΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠ΅ΠΎΡΠ΅ΠΌ ΡΠ»ΠΎΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΠΎΠ»Π½ΠΎΠ²ΡΡ
ΡΡΠ½ΠΊΡΠΈΠΉ. Π€ΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΠΎΠ»Ρ, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡΠΈΠ΅ ΠΏΡΠΈ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠΈ Π·Π²ΡΠΊΠ° ΡΠ°ΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠΎΠΉ, ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ ΠΏΡΡΠ΅ΠΌ ΡΠΎΠ²ΠΌΠ΅ΡΡΠ½ΠΎΠ³ΠΎ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΠΈΡΡΠ΅ΠΌΡ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ: Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ; ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΠ±ΠΎΠ»ΠΎΡΠ΅ΠΊ Π² ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΡΡ
; ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ Π²ΡΠ½ΡΠΆΠ΄Π΅Π½Π½ΠΎΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΡΡΠ°ΡΠΈΠΊΠΈ Π΄Π»Ρ ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΠΊΠΈ ΠΏΡΠΈ Π·Π°Π΄Π°Π½Π½ΡΡ
Π³ΡΠ°Π½ΠΈΡΠ½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΡΡ
, ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΡΠΎΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΠΎΠ»Π΅ΠΉ Π½Π° Π³ΡΠ°Π½ΠΈΡΠ°Ρ
ΡΠ°Π·Π΄Π΅Π»Π° ΠΌΠ½ΠΎΠ³ΠΎΡΠ²ΡΠ·Π½ΡΡ
ΠΎΠ±Π»Π°ΡΡΠ΅ΠΉ ΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ»ΠΎΠ²ΠΈΡΡ
.Π Π΅ΡΠ΅Π½ΠΈΠ΅ Π·Π°Π΄Π°ΡΠΈ ΡΠ²Π΅Π΄Π΅Π½ΠΎ ΠΊ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π±Π΅ΡΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
Π°Π»Π³Π΅Π±ΡΠ°ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π½Π΅ΠΈΠ·Π²Π΅ΡΡΠ½ΡΡ
ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ² ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΠΉ ΠΏΠΎΠ»Π΅ΠΉ Π² ΡΡΠ΄Ρ ΠΏΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΡΠΌ ΡΡΠ½ΠΊΡΠΈΡΠΌ.ΠΠ½Π°Π»ΠΈΠ· ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΡΠΈΡΠ»Π΅Π½Π½ΡΡ
ΡΠ°ΡΡΠ΅ΡΠΎΠ², Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π½ΡΡ
Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠΉ, ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» ΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΡ ΡΡΠ΄ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠ΅ΠΉ Π² ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ΅Ρ
Π°Π½ΠΎΠ°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»ΡΠΌΠΈ Π² ΡΠΎΡΡΠ°Π²Π΅ ΠΏΠ»ΠΎΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ. ΠΡΠΈ ΡΡΠΎΠΌ ΡΡΡΠ΅Π½Ρ: Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ; Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ ΠΈ ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΠΎ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠΌΡ ΠΏΠΎΠ»Ρ; ΡΡΠ΅ΠΏΠ΅Π½Ρ Π½Π°ΡΡΡΠ΅Π½ΠΈΡ ΡΠ°Π΄ΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π½Π°Π³ΡΡΠΆΠ΅Π½ΠΈΡ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ ΠΎΡ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ; ΠΌΠ½ΠΎΠ³ΠΎΠΌΠΎΠ΄ΠΎΠ²ΠΎΡΡΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ Π² ΡΠΎΡΡΠ°Π²Π΅ ΠΏΠ»ΠΎΡΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΠΈ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΏΠ΅ΡΠ΅ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΠΌΠ΅ΠΆΠ΄Ρ ΠΌΠΎΠ΄Π°ΠΌΠΈ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ ΠΎΡ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π½Π°ΡΡΡΠ΅Π½ΠΈΡ ΡΠ°Π΄ΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π½Π°Π³ΡΡΠΆΠ΅Π½ΠΈΡ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ
ΠΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ»ΡΡΠ°ΠΉ ΡΡΠ°ΠΏΠ½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ ΠΎΡΡΠΎΡΠΎΠΏΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠΈΠΈ ΠΏΠ΅ΡΠ΅Π½ΠΈ
Hepatic artery thrombosis (HAT) following liver transplantation (LT) is a severe life-threatening complication that can lead to graft loss and mortality after LT. According to different reports, HAT incidence ranges from 2% to 9%. Modern endovascular and radiosurgical techniques allow for minimally invasive liver graft revascularization. Nonetheless, a major consequence of even a successful revascularization is ischemic cholangiopathy, which can lead to ischemic biliary strictures and anastomotic leak. The paper presents a clinical case of long-term complex treatment of combined complications of LT using minimally invasive endovascular and endoscopic techniques.Π’ΡΠΎΠΌΠ±ΠΎΠ· Π°ΡΡΠ΅ΡΠΈΠΈ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠ° ΠΏΠ΅ΡΠ΅Π½ΠΈ - ΡΡΠΆΠ΅Π»ΠΎΠ΅ ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠ΅, ΠΊΠΎΡΠΎΡΠΎΠ΅ ΠΌΠΎΠΆΠ΅Ρ ΠΏΡΠΈΠ²Π΅ΡΡΠΈ ΠΊ ΠΏΠΎΡΠ΅ΡΠ΅ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠ° ΠΈ ΡΠΌΠ΅ΡΡΠΈ ΡΠ΅ΡΠΈΠΏΠΈΠ΅Π½ΡΠ°. ΠΠΎ Π΄Π°Π½Π½ΡΠΌ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π°Π²ΡΠΎΡΠΎΠ², ΡΠ°ΡΡΠΎΡΠ° Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ ΡΡΠΎΠΌΠ±ΠΎΠ·ΠΎΠ² ΠΊΠΎΠ»Π΅Π±Π»Π΅ΡΡΡ ΠΎΡ 2 Π΄ΠΎ 9%. Π‘ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠ΅ ΡΠ½Π΄ΠΎΠ²Π°ΡΠΊΡΠ»ΡΡΠ½ΡΠ΅ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΡ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ ΠΌΠ°Π»ΠΎΠΈΠ½Π²Π°Π·ΠΈΠ²Π½ΠΎ Π²ΡΠΏΠΎΠ»Π½ΠΈΡΡ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΡ ΠΏΠ΅ΡΠ΅Π½ΠΎΡΠ½ΠΎΠ³ΠΎ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠ°. Π ΡΠΎ ΠΆΠ΅ Π²ΡΠ΅ΠΌΡ ΡΠ΅ΡΡΠ΅Π·Π½ΡΠΌ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠ΅ΠΌ Π΄Π°ΠΆΠ΅ ΡΡΠΏΠ΅ΡΠ½ΠΎΠΉ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠ°Ρ Ρ
ΠΎΠ»Π°Π½Π³ΠΈΠΎΠΏΠ°ΡΠΈΡ, ΠΊΠΎΡΠΎΡΠ°Ρ ΠΌΠΎΠΆΠ΅Ρ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡΡ ΠΊ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
Π±ΠΈΠ»ΠΈΠ°ΡΠ½ΡΡ
ΡΡΡΠΈΠΊΡΡΡ ΠΈ Π½Π΅ΡΠΎΡΡΠΎΡΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ Π°Π½Π°ΡΡΠΎΠΌΠΎΠ·Π°. Π ΡΡΠ°ΡΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ»ΡΡΠ°ΠΉ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ ΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠΈΠΈ ΠΏΠ΅ΡΠ΅Π½ΠΈ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ°Π»ΠΎΠΈΠ½Π²Π°Π·ΠΈΠ²Π½ΡΡ
ΡΠ½Π΄ΠΎΠ²Π°ΡΠΊΡΠ»ΡΡΠ½ΡΡ
ΠΈ ΡΠ½Π΄ΠΎΡΠΊΠΎΠΏΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ
FEATURES OF ELECTROMECHANICAL ACOUSTIC ENERGY CONVERSION BY CYLINDRICAL PIEZOCERAMIC TRANSDUCERS WITH INTERNAL SCREENS IN COMPOSITION OF FLAT SYSTEMS
The problem of sound emission is considered by a system formed from cylindrical piezoceramic radiators with internal acoustically soft screens. Longitudinal axis of emitters lie in one plane. This system is characterized by the interaction of electric, mechanical and acoustic fields in the process of conversion electrical energy to acoustical energy and acoustic fields in the process of forming them in the environments. The purpose of the work is to determine the peculiarities of the electromechanical acoustic transformation of energy by cylindrical piezoceramic radiators with internal screens in the composition of flat systems, taking into account all types of interaction.The research was carried out by the method of bound fields in multiply connected domains with the use of addition theorems for the cylindrical wave functions. The physical fields arising from the emission of sound by such a system are determined by the joint solution of the system of differential equations: the wave equation; equations of motion of thin piezoceramic shells with circular polarization in displacements; the equations of forced electrostatics for piezoceramics at given boundary conditions, the conditions of conjugation of fields at the boundaries of the division of domains and electric conditions.The solution of the problem is reduced to the solution of an infinite system of linear algebraic equations with respect to unknown coefficients of field expansions.An analysis of the results of numerical calculations, performed on the basis of the obtained analytical relations, called to establish a number of features in the electromechanical acoustic transformation of energy by emitters in the composition of flat systems. They include: the role of acoustic interaction in the process of energy conversion; determination of the mechanism of quantitative assessment of the influence of interaction on these processes; the dependence of the degree of violation of the radial symmetry of the acoustic loading of the emitters on the amount of acoustic interaction; the appearance of multimodality of the mechanical field of emitters in the structure of the plane system and the dependence of the redistribution of energy between all modes on the degree of disturbance of the radial symmetry of the acoustic loading of the emitters